and let \(n_C\)  become large, stationary properties such as trajectories
\(\left( \bar{\eta } , \bar{n} / n_C \right)\)  become asymptotically
independent of \(n_C\) . In that case the effective potential separates
into scale and structure components [1]} as
\(\Xi \! \left( {\rm n}\right)& =n_C \int ^{{\rm n}} \bar{\eta } \, d\left( \bar{n} / n_C \right) \equiv n_C \int ^x \bar{\eta } \, d\bar{x}\equiv n_C \hat{\Xi } \! \left( x \right) .\) 
